Abstract
The indirect Coulomb energy for particles of charge e is usually approximated by E ≈ -Ce 2 3 ∫ ρ{variant}(x) 4 3d(x), where ρ{variant}(x) is the single-particle charge density. We prove that, for a suitable constant C, this form for E is actually a universal lower bound.
Original language | English (US) |
---|---|
Pages (from-to) | 444-446 |
Number of pages | 3 |
Journal | Physics Letters A |
Volume | 70 |
Issue number | 5-6 |
DOIs | |
State | Published - Apr 2 1979 |
All Science Journal Classification (ASJC) codes
- General Physics and Astronomy